- Anderson, T;
- Anderssen, E;
- Askins, M;
- Bacon, AJ;
- Bagdasarian, Z;
- Baldoni, A;
- Barros, N;
- Bartoszek, L;
- Bergevin, M;
- Bernstein, A;
- Blucher, E;
- Boissevain, J;
- Bonventre, R;
- Brown, D;
- Callaghan, EJ;
- Cowen, DF;
- Dazeley, S;
- Diwan, M;
- Duce, M;
- Fleming, D;
- Frankiewicz, K;
- Gooding, DM;
- Grant, C;
- Juechter, J;
- Kaptanoglu, T;
- Kim, T;
- Klein, JR;
- Kraus, C;
- Kroupová, T;
- Land, B;
- Lebanowski, L;
- Lozza, V;
- Marino, A;
- Mastbaum, A;
- Mauger, C;
- Mayers, G;
- Minock, J;
- Naugle, S;
- Newcomer, M;
- Nikolica, A;
- Gann, GD Orebi;
- Pickard, L;
- Ren, L;
- Rincon, A;
- Rowe, N;
- Saba, J;
- Schoppmann, S;
- Sensenig, J;
- Smiley, M;
- Song, H;
- Steiger, H;
- Svoboda, R;
- Tiras, E;
- To, WH;
- Trzaska, WH;
- Van Berg, R;
- Veeraraghavan, V;
- Wallig, J;
- Wendel, G;
- Wetstein, M;
- Wurm, M;
- Yang, G;
- Yeh, M;
- Zimmerman, ED
Eos is a technology demonstrator, designed to explore the capabilities of hybrid event detection technology, leveraging both Cherenkov and scintillation light simultaneously. With a fiducial mass of four tons, Eos is designed to operate in a high-precision regime, with sufficient size to utilize time-of-flight information for full event reconstruction, flexibility to demonstrate a range of cutting edge technologies, and simplicity of design to facilitate potential future deployment at alternative sites. Results from Eos can inform the design of future neutrino detectors for both fundamental physics and nonproliferation applications. This paper describes the conceptual design and potential applications of the Eos detector.